Physics 111 Lab #2:
Force and Newton's Laws
Force probes will be used to study the forces
exerted by a cart and other objects in the presence of gravitational,
spring, frictional, and tension forces (see Lectures
4,
5,
6).
Key Activities:
Measuring Weight
with a Force Probe
The relationship between weight and mass will be studied by hanging
a series of masses on the force probe (Lectures
4,
5).
Tension and Acceleration of
a Coupled Two-Mass System
The tension and acceleration
of a "frictionless" cart coupled to a hanging mass will be studied using a
motion detector and a force probe mounted on the cart (Lecture
5).
A comparison of the tension between the cart and
hanging mass (top) and the acceleration of the cart/hanging mass system
(bottom), both when the coupled system is stationary (time < 2 sec) and
when the system is allowed to accelerate (time > 2 sec). Notice that the
tension between the cart and hanging mass becomes smaller when the cart
is released and allowed to accelerate.
What's happening?
Relationship
between Force and a Varying Acceleration
A force probe and motion
detector, in conjunction with an oscillating hanging mass on a spring,
will be used to investigate the relationship between force and
acceleration (Lecture
4).
The results for an oscillating 0.35 kg mass
illustrate the proportionality between the force on the mass (top),
as measured by the force probe, and the acceleration of the mass
(middle) measured by the motion detector. The lower plot shows the
proportionality constant, m=F/a, which in this example has an average
value of 0.37 kg, in rough agreement with the measured mass of the
block + spring. When determining the average value, we ignore the
"spikes" in the ratio F/a caused when both the force and acceleration
approach zero and the value of F/a becomes erratic.
Hooke's Law and the
Spring Constant
A motion detector, a cart equipped
with a force probe, a spring, and a hanging mass will be used to study
Hooke's Law for springs (Lecture
5).
The force exerted by a
spring, F, as measured by the force probe, versus the extension of the
spring, x, illustrating Hooke's force law, F = - k x, and the
determination of the force constant for the spring, k (see Lecture
5).